The high-field side (HFS) scrape-off layer (SOL) is an often under-diagnosed region of tokamak plasmas. Situated in a region with favorable curvature, the HFS SOL has minimal turbulence-induced radial transport compared to the low-field side. Using profile reflectometry, the HFS SOL density profile is measured with high temporal resolution for a wide range of DIII-D plasma discharges for the first time. The magnetic configuration, particularly the location of the secondary separatrix (SS) largely determines the HFS SOL density profile. Additionally, density perturbations induced by edge-localized modes (ELMs) are observed in the HFS SOL, and the impact of ELMs on the SOL density profile is characterized for a range of magnetic configurations. It is found that ELM-induced HFS SOL perturbations are generally localized to within the SS and ELM-induced changes to the HFS wall density are minimized in near double-null configurations. The characterization of the HFS SOL density profile on DIII-D is crucial for the effective coupling of the planned HFS lower hybrid current drive (LHCD) launcher. Experimental HFS SOL measurements are used as input to full-wave simulations of LHCD coupling. This work simulates the effect of the magnetic configuration on LHCD coupling. It also simulates LHCD coupling in ELMs and high qmin discharges. During such discharges, the LHCD coupling is predicted to be resilient to ELM-induced SOL density perturbations.
This paper measures the high-field side (HFS) scrape-off layer (SOL) density profile in DIII-D tokamak, which is crucial for effective coupling of the planned HFS lower hybrid current drive (LHCD) launcher. It shows that the magnetic configuration and edge-localized modes (ELMs) significantly impact the HFS SOL density profile, and simulations predict LHCD coupling to be resilient to ELM-induced density perturbations.